Page 221 - INTRODUCTION TO THE CALCULUS OF VARIATIONS
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208                                            Solutions to the Exercises

                       Exercise 4.3.2. This is a classical result.
                          (i) We start by choosing ψ ∈ C  ∞  (0, 1), ψ ≥ 0,so that
                                                     0
                                               Z  1              1
                                                  r n−1 ψ (r) dr =                     (7.18)
                                                0               σ n−1

                       where σ n−1 = meas (∂B 1 (0)).We then let ψ ≡ 0 outside of (0, 1) and we define
                       for every  > 0
                                                            µ   ¶
                                                         1    |x|
                                                ϕ (x)=    ψ       .
                                                         n

                                     n                  o
                                            n
                          (ii) Let Ω   = x ∈ R : B   (x) ⊂ Ω .Let x ∈ Ω   , the function y → ϕ (x − y)

                       has then its support in Ω since supp ϕ ⊂ B   (0). We therefore have

                        Z                      Z                        Z               µ   ¶
                                                                      1                  |y|
                             u (y) ϕ (x − y) dy =  u (x − y) ϕ (y) dy =  n    u (x − y) ψ     dy


                          R n                    R n                      |y|<
                              Z                         Z  1  Z
                            =       u (x −  z) ψ (|z|) dz =      u (x −  ry) ψ (r) r n−1 drdσ (y) .
                                |z|<1                     0  |y|=1
                                                                                       (7.19)
                       We next use the mean value formula
                                           Z                  Z
                                      1                   1
                           u (x)=                 udσ =            u (x + ry) dσ (y) .  (7.20)
                                  σ n−1 r n−1  ∂B r (x)  σ n−1  |y|=1
                       Returning to (7.19) and using (7.18) combined with (7.20), we deduce that

                                                   Z
                                            u (x)=    u (y) ϕ (x − y) dy .

                                                    R n
                                      n
                       Since ϕ ∈ C  ∞  (R ), we immediately get that u ∈ C ∞  (Ω   ).Since   is arbitrary,
                                  0
                       we find that u ∈ C  ∞  (Ω), as claimed.
                                                      α
                       Exercise 4.3.3. Let V (r)= |log r| and
                                               u (x 1 ,x 2 )= x 1 x 2 V (|x|) .

                       A direct computation shows that

                                             2                                  2
                                            x x 2                            x 1 x 2
                                             1
                                                                                   0
                               = x 2 V (|x|)+     0             = x 1 V (|x|)+   V (|x|)
                            u x 1               V (|x|) and u x 2
                                             |x|                              |x|
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